knitr::opts_chunk$set(echo = TRUE)
library("ggplot2")
library("R.matlab")
library("reshape2") 
library("pracma") 
library("plot.matrix")
library("MASS")
library("ggcorrplot")
library("cowplot")
library("corrplot")
library("Rfast")
library("factoextra")
library("gridExtra")

# Global variables
N <- 240
V <- 441
x1 <- 21
x2 <- 21
nsrcs <- 6

Question 1.1

# function that generate TCs
generateTC <- function(ones_onsets, DO, timeseries) 
{
    stim <- numeric(timeseries)
    for(i in 1:length(ones_onsets))
    {
        stim[(ones_onsets[i]+1):(DO+ones_onsets[i])] <- c(replicate(DO,1))
    }
    return(stim)
}
AV <- c(0, 20, 0, 0, 0, 0)
IV <- c(30, 45, 60, 40, 40, 40)
DO <- c(15, 20, 25, 15, 20, 25)
TC <- matrix(0, nrow = 240, ncol = 6)
# Generate TCs
for (i in 1:6) {
  TC[,i] <- generateTC(seq(AV[i], N, by = IV[i]), DO[i], N)[1:N]
}

TC <- data.frame(TC)
par(mfrow=c(3,2))

# Standardize TC and plot TCs
for (i in 1:6)
{
  TC[,i] <- (TC[,i] - mean(TC[,i])) / sd(TC[,i]);
  plot(TC[, i], typ="l", main=paste("TC", i), ylab=paste("Temporal Source", i))
}

Question 1.2

corrplot(cor(TC), method = 'color', order = 'alphabet', title="\nCorrelation Matrix", type = "lower", tl.srt = 30)

Question 1.3

# Construct tmpSM
tmpSM <- array(0, c(6, 21, 21))
tmpSM[1, 2:6, 2:6] = 1
tmpSM[2, 2:6, 15:19] = 1
tmpSM[3, 8:13, 2:6] = 1
tmpSM[4, 8:13, 15:19] = 1
tmpSM[5, 15:19, 2:6] = 1
tmpSM[6, 15:19, 15:19] = 1

# Plot SMs in six subplots
par(mfrow=c(2, 3))
for (i in 1:6)
{
  plot(tmpSM[i,,], main=paste("tmpSM",i), xlab=NA, ylab=NA, border=NA)
}

# plot 6 vectored SMs to show independence
SM <- matrix(c(c(tmpSM[1,,]), c(tmpSM[2,,]), c(tmpSM[3,,]), c(tmpSM[4,,]), c(tmpSM[5,,]), c(tmpSM[6,,])), 6, 21*21, byrow=TRUE)

corrplot(cor(t(SM)), main="\nSM Correlation Heatmap", method="color")

Question 1.4

# Construct Gamma t and Gamma s
set.seed(10)
Gamma_t = matrix(rnorm(240*6, mean=0, sd=0.25**0.5), 240, 6)
Gamma_s = matrix(rnorm(6*441, mean=0, sd=0.015**0.5), 6, 441)

# Plot correlation
par(mfrow=c(1, 2))
corrplot(cor(Gamma_t), main="\n\n\n\nTemporal Noise", 
         xlab=NA, ylab=NA, method="color")
corrplot(cor(t(Gamma_s)), main="\n\n\n\nSpatial Noise", 
         xlab=NA, ylab=NA, method="color")

df = data.frame(c(Gamma_t))
# Plot histogram of both noise source
gamma_t_plot <- ggplot(df, aes(c(c.Gamma_t.)))+
  geom_histogram(aes(y=..density..),
  binwidth=0.15, color="darkblue", fill="lightblue") +
  labs(title="Distribution of Temporal Noise",x="Value", y = "Density") +
  stat_function(fun = dnorm, args = list(mean = 0, sd = (0.25)**0.5)) +
  geom_vline(xintercept = (1.96)*(0.25)**0.5, color="red") + 
  geom_vline(xintercept = -(1.96)*(0.25)**0.5, color="red")

df = data.frame(c(Gamma_s))
gamma_s_plot <-ggplot(df, aes(c(c.Gamma_s.)))+
  geom_histogram(aes(y=..density..),
  binwidth=0.05, color="darkblue", fill="lightblue") +
  labs(title="Distribution of Spatial Noise",x="Value", y = "Density") +
  stat_function(fun = dnorm, args = list(mean = 0, sd = (0.015)**0.5)) +
  geom_vline(xintercept = (1.96)*(0.015)**0.5, color="red") + 
  geom_vline(xintercept = -(1.96)*(0.015)**0.5, color="red")

plot_grid(gamma_t_plot, gamma_s_plot)

Gamma_ts <- Gamma_t%*%Gamma_s
# Check correlation of the product of Gamma t and Gamma s
corr <- cor(Gamma_ts)

# Randomly sample 10 variables to visualise
samples <- sample (c(1:441), size=10, replace=F)
corrplot(corr[samples, samples], method="color", main="\nCorrelation between 441 variables (Sampled)", type = "lower", tl.srt = 30)

Question 1.5

# Generate a synthetic dataset X
TC <- as.matrix(TC, 6, 240)
X <- (TC + Gamma_t) %*% (SM + Gamma_s)

# Check compatibility
c(dim(TC), dim(Gamma_s))
[1] 240   6   6 441
c(dim(Gamma_t), dim(SM))
[1] 240   6   6 441
dim(X)
[1] 240 441
# Plot at least 100 randomly selected time-series from X
samples <- data.frame(n=1:240, X[, sample.int(240, 100)])
samples <- melt(samples, id.vars = "n")
ggplot(samples, aes(x=n, y=value, col=variable)) + geom_line() + 
  labs(title="100 Ramdonly Selected Time-series", x="", y="Value") +
  theme(plot.margin = margin(1.5,.5,1.5,.5, "cm"),
        legend.key.height= unit(0.1, 'cm'),
        legend.key.width= unit(0.1, 'cm'))

# plot variance of all 441 variables
variances <- colVars(X)
variances <- data.frame(n=1:441, variances)
ggplot(variances, aes(x=n, y=variances)) +geom_point(color="steelblue") + 
  labs(title="Variance of 441 variables", x="Variables", y="Variances")

# Standardize X
X = scale(X)

Question 2.1

D <- as.matrix(TC)

# Estimate A using least square estimation
A_lsr <- abs(solve(t(D)%*%D)%*%t(D)%*%X)

# Calculate D_lsr
D_lsr <- X%*%t(A_lsr)
pal <- colorRampPalette(c("blue", "yellow"))
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(2.5,5))
par(mar = c(2,5,1.5,1.5))
for (i in 1:6) 
{
  A_lsr_p <- A_lsr[i,]
  D_lsr_p <- D_lsr[,i]
  dim(A_lsr_p) <- c(21, 21)
  plot(A_lsr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("Retrieved Spatial Map",i))
  
  plot(D_lsr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("Retrieved Time Course",i))
}

df <- data.frame(D_lsr[,3], X[,30])
colnames(df) <- c("D_lsr_3", "X_30")
plot_1 <- ggplot(df, aes(y=D_lsr_3, x=X_30)) + geom_point(color = "steelblue") +
  labs(title=expression(paste(D[lsr], "  column 3 vs X column 30")),
       x=expression(paste(D[lsr], " column 3")), y = "X column 30") + geom_smooth()

df <- data.frame(D_lsr[,4], X[,30])
colnames(df) <- c("D_lsr_4", "X_30")
plot_2 <- ggplot(df, aes(y=D_lsr_4, x=X_30)) + geom_point(color = "steelblue") +
  labs(title=expression(paste(D[lsr], "  column 4 vs X column 30")),
       x=expression(paste(D[lsr], " column 4")), y = "X column 30") + geom_smooth()

suppressMessages(plot_grid(plot_1, plot_2))

Question 2.2

lambda <- 0.5
I <- matrix(0, 6, 6)
diag(I) <- 1
# Compute scalar value
penalty_term <- lambda * V
# Estimate A_rr and D_rr
A_rr <- abs(solve(t(D)%*%D + penalty_term*I)%*%t(D)%*%X)
D_rr <- X%*%t(A_rr)

C_tlsr = 0
C_trr = 0
for (i in 1:6)
{
  C_tlsr[i] = cor(TC[,i], D_lsr[,i])
  C_trr[i] = cor(TC[,i], D_rr[,i])
}

# Compare the sum of these two correlation vectors
print(paste("Sum of C_tlsr:", sum(C_tlsr)))
[1] "Sum of C_tlsr: 5.09748114621307"
print(paste("Sum of C_trr:", sum(C_trr)))
[1] "Sum of C_trr: 5.16285782879284"
# Set lambda value as 1000 for plot visualisation
lambda <- 1000
# Compute scalar value
penalty_term <- lambda * V
# Estimate A_rr and D_rr
A_rr_1000 <- abs(solve(t(D)%*%D + penalty_term*I)%*%t(D)%*%X)

# plot and compare the shrinkage of variables
values <- data.frame(n=1:441, val=A_lsr[1,])
A_lsr_plot <- ggplot(values, aes(x=n, y=val)) +
  geom_point(color = "steelblue") + 
  labs(title=expression(A[lsr]), y="Values", x="Index")

values <- data.frame(n=1:441, val=A_rr_1000[1,])
A_rr_plot <- ggplot(values, aes(x=n, y=val)) +
  geom_point(color = "steelblue") + 
  labs(title=expression(paste(A[rr], "   ", lambda, " = 1000")), y="Values",
       x="Index")

suppressMessages(plot_grid(A_lsr_plot, A_rr_plot))

Question 2.3

# Select ρ between 0 and 1 with an interval of 0.05
rho_values <- seq(from=0, to=1, by=0.05)
MSE <- rep(0, 21)
for (j in 1:21)
{
  rho <- rho_values[j]
  step <- 1/(norm(TC %*% t(TC)) * 1.1)
  thr <- rho*N*step
  Ao <- matrix(0, nsrcs, 1)
  A <- matrix(0, nsrcs, 1)
  Alr <- matrix(0, nsrcs, x1*x2)
  MSE_temp <- rep(0, 10)
  
  # Generate new standardized X in terms of Gamma t and Gamma s
  for (a in 1:10) {
    set.seed(a)
    Gamma_t_temp = matrix(rnorm(240*6, mean=0, sd=0.25**0.5), 240, 6)
    Gamma_s_temp = matrix(rnorm(6*441, mean=0, sd=0.015**0.5), 6, 441)
    X_temp <- (TC + Gamma_t_temp) %*% (SM + Gamma_s_temp)
    X_temp <- scale(X_temp)
    
    for (k in 1:(x1*x2)) {
      A <- Ao+step*(t(TC) %*% (X_temp[,k]-(TC%*%Ao)))
      A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
      
      for (i in 1:10) {
        Ao <- A
        A <- Ao+step * (t(TC)%*%(X_temp[,k]-(TC%*%Ao)))
        A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
        }
      Alr[,k] <- A
    }
    Alr <- Alr
    Dlr <- X_temp%*%t(Alr)
    MSE_temp[a] <- norm((X_temp - Dlr%*%Alr), type='F')^2/(N*V)
  }
  
  # Compute the average MSE of the current ρ
  MSE[j] <- mean(MSE_temp)
}
# plot average of MSE over these 10 realizations against each value of ρ

df <- data.frame(rho_values, MSE)
plot_1 <- ggplot(df, aes(x=rho_values, y=MSE)) + geom_point(color="steelblue") +
  labs(title="Average MSE for each ρ", x="ρ values", y="Average MSE")

df <- df[10:21,]
plot_2 <- ggplot(df, aes(x=rho_values, y=MSE)) + geom_point(color="steelblue") +
  labs(title="Average MSE for each ρ (Zoomed In)", x="ρ values", y="Average MSE")

suppressMessages(plot_grid(plot_1, plot_2))

Question 2.4

# Estimate A_lr and D_lr using the selected ρ value
rho <- 0.6
step <- 1/(norm(TC %*% t(TC)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_lr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(TC) %*% (X[,k]-(TC%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(TC)%*%(X[,k]-(TC%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_lr[,k] <- A
}
A_lr <- abs(A_lr)
D_lr <- X%*%t(A_lr)
# estimate four correlation vectors
C_trr <- 0
C_srr <- 0
C_tlr <- 0
C_slr <- 0

for (i in 1:6)
{
  C_trr[i] = cor(TC[,i], D_rr[,i])
  C_tlr[i] = cor(TC[,i], D_lr[,i])
  C_srr[i] = cor(SM[i,], A_rr[i,])
  C_slr[i] = cor(SM[i,], A_lr[i,])  
}
sum(C_trr)
[1] 5.162858
sum(C_tlr)
[1] 5.294203
sum(C_srr)
[1] 3.388821
sum(C_slr)
[1] 5.043101
layout(matrix(seq(from=1, to=24, by=1), 6, 4, ncol = 4), 
       widths=c(3,5, 3, 5))
par(mar = c(3,5,1.5,2))
for (i in 1:6) {
  A_rr_p <- A_rr[i,]
  A_lr_p <- A_lr[i,]
  dim(A_rr_p) <- c(21, 21)
  dim(A_lr_p) <- c(21, 21)
  plot(A_rr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, main=paste("Arr",i))
  plot(D_rr[,i], xlab=NA, ylab=NA, main=paste("Drr",i), 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, col="blue", type="l")
  plot(A_lr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, main=paste("Alr",i))
  plot(D_lr[,i], xlab=NA, ylab=NA, main=paste("Dlr",i),
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, col="blue", type="l")
}

Question 2.5 using SVD


pcr <- svd(D)
Z <- pcr$u
par(mfrow=c(6, 2), mar = c(2,3,1.5,2))

# Plot the regressors in Z and source TCs side by side
for (i in 1:6) {
  plot(TC[,i], type="l", main=paste("TC", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
  plot(Z[,i], type="l", main=paste("Z", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
}

ev <- pcr$d
ev <- data.frame(index=seq(1, 6), ev)
plot(ev, col="blue", main="Eigenvalues of each PC", xlab="PCs", ylab="Eigenvalues",
     cex.main=1.4, cex.lab=1.4, cex.axis=1.4)

# Estimate A_pcr and D_pcr using the ρ = 0.001
matrix <- Z
rho <- 0.001
step <- 1/(norm(Z %*% t(Z)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_pcr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(matrix) %*% (X[,k]-(matrix%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(matrix)%*%(X[,k]-(matrix%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_pcr[,k] <- A
}
A_pcr <- abs(A_pcr)
D_pcr <- X%*%t(A_pcr)
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(0.8,2))
par(mar = c(2,5,1.5,1.5))

# Plot the results of DPCR and APCR side by side
for (i in 1:6) 
{
  A_pcr_p <- A_pcr[i,]
  D_pcr_p <- D_pcr[,i]
  dim(A_pcr_p) <- c(21, 21)
  plot(A_pcr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("A pcr",i))
  
  plot(D_pcr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("D pcr",i))
}

Question 2.5 using PRCOMP

m <- prcomp(D, center = TRUE, scale.=TRUE)
Z <- m$x
pev <- fviz_eig(m) + 
  labs(title="Percent of explained variances of PCs", x="PCs")
eigenvalues <- fviz_eig(m, choice="eigenvalue", geom="line") + 
  labs(title="Eigenvalue of each PC", x="PCS")
suppressMessages(plot_grid(pev, eigenvalues))

par(mfrow=c(6, 2), mar = c(2,3,1.5,2))

# Plot the regressors in Z and source TCs side by side
for (i in 1:6) {
  plot(TC[,i], type="l", main=paste("TC", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
  plot(Z[,i], type="l", main=paste("Z", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
}

# Estimate A_pcr and D_pcr using the ρ = 0.001
matrix <- Z
rho <- 0.001
step <- 1/(norm(Z %*% t(Z)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_pcr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(matrix) %*% (X[,k]-(matrix%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(matrix)%*%(X[,k]-(matrix%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_pcr[,k] <- A
}
A_pcr <- abs(A_pcr)
D_pcr <- X%*%t(A_pcr)
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(0.8,2))
par(mar = c(2,5,1.5,1.5))

# Plot the results of DPCR and APCR side by side
for (i in 1:6) 
{
  A_pcr_p <- A_pcr[i,]
  D_pcr_p <- D_pcr[,i]
  dim(A_pcr_p) <- c(21, 21)
  plot(A_pcr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("A pcr",i))
  
  plot(D_pcr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("D pcr",i))
}

df <- data.frame(m$rotation)
df
---
title: "R Notebook"
output: html_notebook
---

```{r}
knitr::opts_chunk$set(echo = TRUE)
library("ggplot2")
library("R.matlab")
library("reshape2") 
library("pracma") 
library("plot.matrix")
library("MASS")
library("ggcorrplot")
library("cowplot")
library("corrplot")
library("Rfast")
library("factoextra")

# Global variables
N <- 240
V <- 441
x1 <- 21
x2 <- 21
nsrcs <- 6
```
# Question 1.1
```{r}
# function that generate TCs
generateTC <- function(ones_onsets, DO, timeseries) 
{
	stim <- numeric(timeseries)
	for(i in 1:length(ones_onsets))
	{
		stim[(ones_onsets[i]+1):(DO+ones_onsets[i])] <- c(replicate(DO,1))
   	}
	return(stim)
}
```

```{r}
AV <- c(0, 20, 0, 0, 0, 0)
IV <- c(30, 45, 60, 40, 40, 40)
DO <- c(15, 20, 25, 15, 20, 25)
TC <- matrix(0, nrow = 240, ncol = 6)
# Generate TCs
for (i in 1:6) {
  TC[,i] <- generateTC(seq(AV[i], N, by = IV[i]), DO[i], N)[1:N]
}

TC <- data.frame(TC)
```

```{r, echo=TRUE, fig.height=3.5, fig.width=3.8}
par(mfrow=c(3,2))

# Standardize TC and plot TCs
for (i in 1:6)
{
  TC[,i] <- (TC[,i] - mean(TC[,i])) / sd(TC[,i]);
  plot(TC[, i], typ="l", main=paste("TC", i), ylab=paste("Temporal Source", i))
}
```
# Question 1.2
```{r}
corrplot(cor(TC), method = 'color', order = 'alphabet', title="\nCorrelation Matrix", type = "lower", tl.srt = 30)
```
# Question 1.3
```{r, echo=TRUE, fig.height=2.5, fig.width=4}
# Construct tmpSM
tmpSM <- array(0, c(6, 21, 21))
tmpSM[1, 2:6, 2:6] = 1
tmpSM[2, 2:6, 15:19] = 1
tmpSM[3, 8:13, 2:6] = 1
tmpSM[4, 8:13, 15:19] = 1
tmpSM[5, 15:19, 2:6] = 1
tmpSM[6, 15:19, 15:19] = 1

# Plot SMs in six subplots
par(mfrow=c(2, 3))
for (i in 1:6)
{
  plot(tmpSM[i,,], main=paste("tmpSM",i), xlab=NA, ylab=NA, border=NA)
}
```

```{r, echo=TRUE, fig.height=2.5, fig.width=2.5}
# plot 6 vectored SMs to show independence
SM <- matrix(c(c(tmpSM[1,,]), c(tmpSM[2,,]), c(tmpSM[3,,]), c(tmpSM[4,,]), c(tmpSM[5,,]), c(tmpSM[6,,])), 6, 21*21, byrow=TRUE)

corrplot(cor(t(SM)), main="\nSM Correlation Heatmap", method="color")
```
# Question 1.4
```{r, echo=TRUE, fig.height=3, fig.width=5}
# Construct Gamma t and Gamma s
set.seed(10)
Gamma_t = matrix(rnorm(240*6, mean=0, sd=0.25**0.5), 240, 6)
Gamma_s = matrix(rnorm(6*441, mean=0, sd=0.015**0.5), 6, 441)

# Plot correlation
par(mfrow=c(1, 2))
corrplot(cor(Gamma_t), main="\n\n\n\nTemporal Noise", 
         xlab=NA, ylab=NA, method="color")
corrplot(cor(t(Gamma_s)), main="\n\n\n\nSpatial Noise", 
         xlab=NA, ylab=NA, method="color")
```

```{r, echo=TRUE, fig.height=2, fig.width=4}
df = data.frame(c(Gamma_t))
# Plot histogram of both noise source
gamma_t_plot <- ggplot(df, aes(c(c.Gamma_t.)))+
  geom_histogram(aes(y=..density..),
  binwidth=0.15, color="darkblue", fill="lightblue") +
  labs(title="Distribution of Temporal Noise",x="Value", y = "Density") +
  stat_function(fun = dnorm, args = list(mean = 0, sd = (0.25)**0.5)) +
  geom_vline(xintercept = (1.96)*(0.25)**0.5, color="red") + 
  geom_vline(xintercept = -(1.96)*(0.25)**0.5, color="red")

df = data.frame(c(Gamma_s))
gamma_s_plot <-ggplot(df, aes(c(c.Gamma_s.)))+
  geom_histogram(aes(y=..density..),
  binwidth=0.05, color="darkblue", fill="lightblue") +
  labs(title="Distribution of Spatial Noise",x="Value", y = "Density") +
  stat_function(fun = dnorm, args = list(mean = 0, sd = (0.015)**0.5)) +
  geom_vline(xintercept = (1.96)*(0.015)**0.5, color="red") + 
  geom_vline(xintercept = -(1.96)*(0.015)**0.5, color="red")

plot_grid(gamma_t_plot, gamma_s_plot)
```

```{r, echo=TRUE, fig.height=3, fig.width=2.5}
Gamma_ts <- Gamma_t%*%Gamma_s
# Check correlation of the product of Gamma t and Gamma s
corr <- cor(Gamma_ts)

# Randomly sample 10 variables to visualise
samples <- sample (c(1:441), size=10, replace=F)
corrplot(corr[samples, samples], method="color", main="\nCorrelation between 441 variables (Sampled)", type = "lower", tl.srt = 30)
```

# Question 1.5
```{r}
# Generate a synthetic dataset X
TC <- as.matrix(TC, 6, 240)
X <- (TC + Gamma_t) %*% (SM + Gamma_s)

# Check compatibility
c(dim(TC), dim(Gamma_s))
c(dim(Gamma_t), dim(SM))
dim(X)
```

```{r}
# Plot at least 100 randomly selected time-series from X
samples <- data.frame(n=1:240, X[, sample.int(240, 100)])
samples <- melt(samples, id.vars = "n")
ggplot(samples, aes(x=n, y=value, col=variable)) + geom_line() + 
  labs(title="100 Ramdonly Selected Time-series", x="", y="Value") +
  theme(plot.margin = margin(1.5,.5,1.5,.5, "cm"),
        legend.key.height= unit(0.1, 'cm'),
        legend.key.width= unit(0.1, 'cm'))
```

```{r, echo=TRUE, fig.height=1.5, fig.width=2.6}
# plot variance of all 441 variables
variances <- colVars(X)
variances <- data.frame(n=1:441, variances)
ggplot(variances, aes(x=n, y=variances)) +geom_point(color="steelblue") + 
  labs(title="Variance of 441 variables", x="Variables", y="Variances")
```
```{r}
# Standardize X
X = scale(X)
```


# Question 2.1
```{r}
D <- as.matrix(TC)

# Estimate A using least square estimation
A_lsr <- abs(solve(t(D)%*%D)%*%t(D)%*%X)

# Calculate D_lsr
D_lsr <- X%*%t(A_lsr)
```

```{r, echo=TRUE, fig.height=4, fig.width=3.5}
pal <- colorRampPalette(c("blue", "yellow"))
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(2.5,5))
par(mar = c(2,5,1.5,1.5))
for (i in 1:6) 
{
  A_lsr_p <- A_lsr[i,]
  D_lsr_p <- D_lsr[,i]
  dim(A_lsr_p) <- c(21, 21)
  plot(A_lsr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("Retrieved Spatial Map",i))
  
  plot(D_lsr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("Retrieved Time Course",i))
}
```

```{r, echo=TRUE, fig.height=1.65, fig.width=4}
df <- data.frame(D_lsr[,3], X[,30])
colnames(df) <- c("D_lsr_3", "X_30")
plot_1 <- ggplot(df, aes(y=D_lsr_3, x=X_30)) + geom_point(color = "steelblue") +
  labs(title=expression(paste(D[lsr], "  column 3 vs X column 30")),
       x=expression(paste(D[lsr], " column 3")), y = "X column 30") + geom_smooth()

df <- data.frame(D_lsr[,4], X[,30])
colnames(df) <- c("D_lsr_4", "X_30")
plot_2 <- ggplot(df, aes(y=D_lsr_4, x=X_30)) + geom_point(color = "steelblue") +
  labs(title=expression(paste(D[lsr], "  column 4 vs X column 30")),
       x=expression(paste(D[lsr], " column 4")), y = "X column 30") + geom_smooth()

suppressMessages(plot_grid(plot_1, plot_2))
```
# Question 2.2
```{r}
lambda <- 0.5
I <- matrix(0, 6, 6)
diag(I) <- 1
# Compute scalar value
penalty_term <- lambda * V
# Estimate A_rr and D_rr
A_rr <- abs(solve(t(D)%*%D + penalty_term*I)%*%t(D)%*%X)
D_rr <- X%*%t(A_rr)

C_tlsr = 0
C_trr = 0
for (i in 1:6)
{
  C_tlsr[i] = cor(TC[,i], D_lsr[,i])
  C_trr[i] = cor(TC[,i], D_rr[,i])
}

# Compare the sum of these two correlation vectors
print(paste("Sum of C_tlsr:", sum(C_tlsr)))
print(paste("Sum of C_trr:", sum(C_trr)))
```

```{r, echo=TRUE, fig.height=1.3, fig.width=4}
# Set lambda value as 1000 for plot visualisation
lambda <- 1000
# Compute scalar value
penalty_term <- lambda * V
# Estimate A_rr and D_rr
A_rr_1000 <- abs(solve(t(D)%*%D + penalty_term*I)%*%t(D)%*%X)

# plot and compare the shrinkage of variables
values <- data.frame(n=1:441, val=A_lsr[1,])
A_lsr_plot <- ggplot(values, aes(x=n, y=val)) +
  geom_point(color = "steelblue") + 
  labs(title=expression(A[lsr]), y="Values", x="Index")

values <- data.frame(n=1:441, val=A_rr_1000[1,])
A_rr_plot <- ggplot(values, aes(x=n, y=val)) +
  geom_point(color = "steelblue") + 
  labs(title=expression(paste(A[rr], "   ", lambda, " = 1000")), y="Values",
       x="Index")

suppressMessages(plot_grid(A_lsr_plot, A_rr_plot))
```
# Question 2.3
```{r}
# Select ρ between 0 and 1 with an interval of 0.05
rho_values <- seq(from=0, to=1, by=0.05)
MSE <- rep(0, 21)
```

```{r}
for (j in 1:21)
{
  rho <- rho_values[j]
  step <- 1/(norm(TC %*% t(TC)) * 1.1)
  thr <- rho*N*step
  Ao <- matrix(0, nsrcs, 1)
  A <- matrix(0, nsrcs, 1)
  Alr <- matrix(0, nsrcs, x1*x2)
  MSE_temp <- rep(0, 10)
  
  # Generate new standardized X in terms of Gamma t and Gamma s
  for (a in 1:10) {
    set.seed(a)
    Gamma_t_temp = matrix(rnorm(240*6, mean=0, sd=0.25**0.5), 240, 6)
    Gamma_s_temp = matrix(rnorm(6*441, mean=0, sd=0.015**0.5), 6, 441)
    X_temp <- (TC + Gamma_t_temp) %*% (SM + Gamma_s_temp)
    X_temp <- scale(X_temp)
    
    for (k in 1:(x1*x2)) {
      A <- Ao+step*(t(TC) %*% (X_temp[,k]-(TC%*%Ao)))
      A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
      
      for (i in 1:10) {
        Ao <- A
        A <- Ao+step * (t(TC)%*%(X_temp[,k]-(TC%*%Ao)))
        A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
        }
      Alr[,k] <- A
    }
    Alr <- Alr
    Dlr <- X_temp%*%t(Alr)
    MSE_temp[a] <- norm((X_temp - Dlr%*%Alr), type='F')^2/(N*V)
  }
  
  # Compute the average MSE of the current ρ
  MSE[j] <- mean(MSE_temp)
}
```

```{r, echo=TRUE, fig.height=2, fig.width=4}
# plot average of MSE over these 10 realizations against each value of ρ

df <- data.frame(rho_values, MSE)
plot_1 <- ggplot(df, aes(x=rho_values, y=MSE)) + geom_point(color="steelblue") +
  labs(title="Average MSE for each ρ", x="ρ values", y="Average MSE")

df <- df[10:21,]
plot_2 <- ggplot(df, aes(x=rho_values, y=MSE)) + geom_point(color="steelblue") +
  labs(title="Average MSE for each ρ (Zoomed In)", x="ρ values", y="Average MSE")

suppressMessages(plot_grid(plot_1, plot_2))
```
# Question 2.4
```{r}
# Estimate A_lr and D_lr using the selected ρ value
rho <- 0.6
step <- 1/(norm(TC %*% t(TC)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_lr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(TC) %*% (X[,k]-(TC%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(TC)%*%(X[,k]-(TC%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_lr[,k] <- A
}
A_lr <- abs(A_lr)
D_lr <- X%*%t(A_lr)
```

```{r}
# estimate four correlation vectors
C_trr <- 0
C_srr <- 0
C_tlr <- 0
C_slr <- 0

for (i in 1:6)
{
  C_trr[i] = cor(TC[,i], D_rr[,i])
  C_tlr[i] = cor(TC[,i], D_lr[,i])
  C_srr[i] = cor(SM[i,], A_rr[i,])
  C_slr[i] = cor(SM[i,], A_lr[i,])  
}
sum(C_trr)
sum(C_tlr)
sum(C_srr)
sum(C_slr)
```

```{r, echo=TRUE, fig.height=5, fig.width=5.5}
layout(matrix(seq(from=1, to=24, by=1), 6, 4, ncol = 4), 
       widths=c(3,5, 3, 5))
par(mar = c(3,5,1.5,2))
for (i in 1:6) {
  A_rr_p <- A_rr[i,]
  A_lr_p <- A_lr[i,]
  dim(A_rr_p) <- c(21, 21)
  dim(A_lr_p) <- c(21, 21)
  plot(A_rr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, main=paste("Arr",i))
  plot(D_rr[,i], xlab=NA, ylab=NA, main=paste("Drr",i), 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, col="blue", type="l")
  plot(A_lr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, main=paste("Alr",i))
  plot(D_lr[,i], xlab=NA, ylab=NA, main=paste("Dlr",i),
       cex.main=1.6, cex.lab=1.5, cex.axis=1.2, col="blue", type="l")
}
```
# Question 2.5 using SVD
```{r, echo=TRUE, fig.height=5, fig.width=6}

pcr <- svd(D)
Z <- pcr$u
par(mfrow=c(6, 2), mar = c(2,3,1.5,2))

# Plot the regressors in Z and source TCs side by side
for (i in 1:6) {
  plot(TC[,i], type="l", main=paste("TC", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
  plot(Z[,i], type="l", main=paste("Z", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
}
```
```{r, echo=TRUE, fig.height=1.5, fig.width=3}
ev <- pcr$d
ev <- data.frame(index=seq(1, 6), ev)
plot(ev, col="blue", main="Eigenvalues of each PC", xlab="PCs", ylab="Eigenvalues",
     cex.main=1.4, cex.lab=1.4, cex.axis=1.4)
```

```{r}
# Estimate A_pcr and D_pcr using the ρ = 0.001
matrix <- Z
rho <- 0.001
step <- 1/(norm(Z %*% t(Z)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_pcr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(matrix) %*% (X[,k]-(matrix%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(matrix)%*%(X[,k]-(matrix%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_pcr[,k] <- A
}
A_pcr <- abs(A_pcr)
D_pcr <- X%*%t(A_pcr)
```

```{r, echo=TRUE, fig.height=4, fig.width=3.5}
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(0.8,2))
par(mar = c(2,5,1.5,1.5))

# Plot the results of DPCR and APCR side by side
for (i in 1:6) 
{
  A_pcr_p <- A_pcr[i,]
  D_pcr_p <- D_pcr[,i]
  dim(A_pcr_p) <- c(21, 21)
  plot(A_pcr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("A pcr",i))
  
  plot(D_pcr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("D pcr",i))
}
```

# Question 2.5 using PRCOMP
```{r, echo=TRUE, fig.height=1.5, fig.width=4}
m <- prcomp(D, center = TRUE, scale.=TRUE)
Z <- m$x
pev <- fviz_eig(m) + 
  labs(title="Percent of explained variances of PCs", x="PCs")
eigenvalues <- fviz_eig(m, choice="eigenvalue", geom="line") + 
  labs(title="Eigenvalue of each PC", x="PCS")
suppressMessages(plot_grid(pev, eigenvalues))
```

```{r, echo=TRUE, fig.height=7, fig.width=6}
par(mfrow=c(6, 2), mar = c(2,3,1.5,2))

# Plot the regressors in Z and source TCs side by side
for (i in 1:6) {
  plot(TC[,i], type="l", main=paste("TC", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
  plot(Z[,i], type="l", main=paste("Z", i), cex.main=1.5, cex.lab=1.5, cex.axis=1.5)
}
```

```{r}
# Estimate A_pcr and D_pcr using the ρ = 0.001
matrix <- Z
rho <- 0.001
step <- 1/(norm(Z %*% t(Z)) * 1.1)
thr <- rho*N*step
Ao <- matrix(0, nsrcs, 1)
A <- matrix(0, nsrcs, 1)
A_pcr <- matrix(0, nsrcs, x1*x2)

for (k in 1:(x1*x2)) {
  A <- Ao+step*(t(matrix) %*% (X[,k]-(matrix%*%Ao)))
  A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  
  for (i in 1:10) {
    Ao <- A
    A <- Ao+step * (t(matrix)%*%(X[,k]-(matrix%*%Ao)))
    A <- (1/(1+thr)) * (sign(A)*pmax(replicate(nsrcs, 0), abs(A)-thr))
  }
  A_pcr[,k] <- A
}
A_pcr <- abs(A_pcr)
D_pcr <- X%*%t(A_pcr)
```

```{r, echo=TRUE, fig.height=4, fig.width=3.5}
layout(matrix(c(1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12), 6, 2, ncol = 2), 
       widths=c(0.8,2))
par(mar = c(2,5,1.5,1.5))

# Plot the results of DPCR and APCR side by side
for (i in 1:6) 
{
  A_pcr_p <- A_pcr[i,]
  D_pcr_p <- D_pcr[,i]
  dim(A_pcr_p) <- c(21, 21)
  plot(A_pcr_p, border=F, col = pal(40), xlab=NA, ylab=NA, 
       main=paste("A pcr",i))
  
  plot(D_pcr_p, type = "l", xlab=NA, ylab=NA, 
       main=paste("D pcr",i))
}
```

```{r}
df <- data.frame(m$rotation)
df
```

